A circuit (10) for reducing errors due to adjacent pixel interdependence in a liquid crystal display includes a decomposer (12) for dividing an input signal into a plurality of signals having at least a high brightness signal and at least one low brightness signal, a delay match circuit (14) for the high brightness signal to provide a delay high brightness signal, one or more transient conditioner circuits (16 and/or 18) for processing the at least one low brightness signal to provide at least one transient conditioned low brightness signal, and a combiner (20) for combining the delay matched high brightness signal with the at least one transient conditioned low brightness signal to provide an output signal having reduced sparkle artifacts.
|
11. A method for reducing declination errors in a liquid crystal display, comprising the steps of:
dividing an input signal into at least high, medium and low brightness signals limiting, including an anticipatory limiting step and a reactive limiting step, signal transients between brightness levels of at least one of said medium and low brightness signals;
delay matching the high brightness signal; and,
combining said at least one limited brightness signal and said delayed high brightness signal to form an output signal having reduced sparkle artifacts.
1. A circuit for reducing declination errors in a liquid crystal display, comprising:
a decomposer for dividing an input signal into a plurality of signals having at least high, medium and low brightness signals;
at least one transient conditioner circuit including an anticipatory portion and a reactive portion for limiting signal transients between brightness levels in at least one of said medium and low brightness signals;
a delay match circuit for said high brightness signal; and,
means for combining the delayed high brightness signal with said at least one signal transient processed brightness signal to provide an output signal, wherein said output signal has reduced sparkle artifacts.
2. The circuit of
3. The circuit of
4. The circuit of
5. The circuit of
6. The circuit of
7. The circuit of
8. The circuit of
9. The circuit of
12. The method of
14. The method of
combining said slew rate limited and finite response filtered signal with said high and low brightness signals.
15. The method of
slew rate limiting and finite response filtering said medium brightness signal; and,
applying different slew rates and different finite filter responses to said medium and low brightness signals.
16. The method of
slew rate limiting and finite response filtering said medium brightness signal; and,
applying different slew rates and different finite filter responses to said medium and low brightness signals.
|
(not applicable)
1. Field of the Invention
This invention relates to the field of video systems utilizing a liquid crystal display (LCD), and in particular, to video systems utilizing normally white liquid crystal on silicon imagers.
2. Description of Related Art
Liquid Crystal on Silicon (LCOS) can be thought of as one large liquid crystal placed over a silicon wafer. The silicon wafer is divided into an incremental array of tiny plates. A tiny incremental region of the liquid crystal is influenced by the electric field generated by each tiny plate and a common plate. Each such tiny plate and corresponding liquid crystal region are together referred to as a cell of the imager. Each cell corresponds to an individually controllable pixel. Each tiny plate is also a mirror for reflecting back a cell's light. A common plate electrode is disposed on the other side of the liquid crystal.
The drive voltages are supplied to plate electrodes on each side of the LCOS array. In the presently preferred LCOS system to which the inventive arrangements pertain, the common plate is always at a potential of 8 volts. Each of the other plates in the array of tiny plates is operated in two voltage ranges. For positive pictures, the voltage varies between 0 volts and 8 volts. For negative pictures the voltage varies between 8 volts and 16 volts.
The light supplied to the imager, and therefore supplied to each cell of the imager, is field polarized. Incoming light is incident upon the common electrode which is transparent. Each liquid crystal cell rotates the polarization of the input light responsive to the RMS value of the electric field applied to the cell by the plate electrodes. Generally speaking, the cells are not responsive to the polarity (positive or negative) of the applied electric field. Rather, the brightness of each pixel's cell is generally only a function of the rotation of the polarization of the light incident on the cell. Furthermore, polarization rotation for each cell is a non-linear function of the electric field. Polarization rotation for a given cell occurs as the light passes through the liquid crystal both before and after reflection from the cell plate. It is the rotation of the polarization that is capable of being controlled. Light leaving the imager is approximately the same intensity, but a different polarization. This may depend on the intensity that is ultimately desired. It should be noted that it is undesirable to have the imager absorbing light because it can get too hot. The imager will get hot due to some spurious amount of absorption.
If adjacent pixels produce different brightness, then there must be a different potential on the 2 cell plates corresponding to the adjacent pixels. When potentials on adjacent cell plates are unequal, there is an electric field between them which is known as a fringing field. The fringing field has some components, which are orthogonal to the desired field. These orthogonal components are not a problem in the space between adjacent mirrors. But, the orthogonal components of the electric field, which is over the mirror, will have the effect of distorting the polarization rotation. This distortion results in a substantial local increase in brightness. This is a particular problem when the pixel is supposed to be dark, but is usually an insignificant problem when the pixels are intended to be bright since the pixels are not very different in voltage so the fringing field is not that great. Also, for dark pixels, the additional brightness is much more noticeable. Contrast ratio is also very important in making a high quality display. It is very important to achieve sufficient black level. A proportionately larger drive voltage is needed to create a slightly darker image in a normally white display. Often, a large difference in voltage between adjacent pixels is needed. This results in a major fringing field that produces a visible artifact denoted sparkle. Due to the rotational effects of the fringing fields, this phenomenon is also referred to as a declination error in the imager. Sparkle artifacts can be red, blue and/or green, but green is usually the most prominent color.
Because of the particular manufacturing process used for many imagers, horizontally adjacent pixels suffer more from the fringing field problem. Thus, a need exists for overcoming the sparkle problem described above.
A circuit for reducing declination errors in a liquid crystal display, in accordance with the inventive arrangements, comprises: a decomposer for dividing an input signal into a plurality of signals having at least a high brightness signal and at least one low brightness signal; at least one transient conditioner circuit for reducing declination errors by limiting signal transients between brightness levels in said at least one low brightness signal; a delay match circuit for said high brightness signal; and, means for combining the delayed high brightness signal with said at least one signal transient processed low brightness signal to provide an output signal, wherein said output signal has reduced sparkle artifacts. The at least one transient conditioner can comprise at least one slew rate limiter and at least one finite response filter.
A method for reducing adjacent pixel interdependence in a liquid crystal display, in accordance with the inventive arrangements, comprises the steps of: dividing an input signal into at least a high brightness signal and at least one low brightness signal; slew rate limiting and finite response filtering the at least one low brightness signal to reduce adjacent pixel interdependence by limiting signal transients between brightness levels; delay matching the high brightness signal; and, combining the at least one slew rate limited and finite response filtered low brightness signal and the delayed high brightness signal to form an output signal having reduced sparkle artifacts.
The method can further comprise the step of slew rate limiting dark going transients of the at least one low brightness level signal and finite response filtering bright going transients of the at least one low brightness level signal. The slew rate limiting can be asymmetric.
The method can further comprise the steps of: further dividing the input signal into a medium brightness signal having brightness levels between the high and low brightness level signals; limiting signal transients between brightness levels of the medium brightness signal to further reduce adjacent pixel interdependence; and, combining the slew rate limited and finite response filtered signal with the high and low brightness signals. The medium brightness signal can be slew rate limited and finite response filtered. Different slew rates and different finite filter responses can be applied to the medium and low brightness signals.
Reducing the difference in brightness between adjacent pixels when they are dark, but not when they are bright can resolve the sparkle problem previously described. A device called a decomposer 12 on the input divides the input signal into at least two signals on a circuit 10 used to reduce adjacent pixel interdependence in liquid crystal displays as shown in FIG. 1. It should be understood that Sparkle or declination errors can also be considered a subset of a broader phenomenon known as adjacent pixel interdependence. It should be noted that the present invention is particularly useful for liquid crystal on silicon (LCOS) displays but is not necessarily limited thereto. The decomposer 12 serves as an amplitude discriminator for the input signal which is preferably an eight (8) bit video signal that preferably carries the desired brightness of one color component (Red, Green, or Blue).
The input signal is decomposed in a manner that enables obtaining the original signal when the decomposed or divided signals are added or combined back together. The method in accordance with the present invention would further process the low brightness portion (L and optionally M) and delay match the high brightness portion (H). Then, the signals are recombined and sent to the imager. The same technique can also be applied to the luminance signal (only need one of these decomposed). Accordingly, the improved approach relies upon one decomposer for each color (Red, Green, & Blue). It should be understood that the decomposer can divide the input signal into two or more component signals within contemplation of the present invention.
The decomposer must have at least two inputs, a threshold input and a brightness input signal. If a single threshold is used and the brightness input signal is below the threshold, then the high output is zero (0) and the low output is the brightness input signal itself. If the brightness input signal is above the threshold, then the high output is the brightness input signal minus the threshold input and the low output is the threshold input signal.
Referring once again to
When the decomposer 12 utilizes only a single threshold signal (Tl for example) and the input signal is below the threshold signal, then the high brightness signal is zero and the low brightness signal is the input signal and if the input signal is above the threshold signal, then the high brightness signal is the input signal minus the threshold signal and the low brightness signal is the threshold signal.
If the decomposer 12 includes a lower threshold and an upper threshold, wherein if the input signal is greater than the upper threshold, then the high brightness signal equals the input signal minus the upper threshold, the medium brightness signal equals the upper threshold minus the lower threshold, and the low brightness signal equals the low threshold, and wherein if the input signal is less than the upper threshold but greater than the lower threshold, then the high brightness signal equals zero, the medium brightness signal equals the input signal minus the lower threshold, and the low brightness signal equals the lower threshold, and wherein if the input signal is less than the lower threshold, then the high brightness signal equals zero, the medium brightness signal equals zero, and the low brightness signal equals the input signal. The scenario above where the decomposer 12 divides the input signal into three signals, a high (H), a medium (M), and a low (L) signal, can be summarized as follows:
Referring to
The reactive part of the transient conditioner 50 consists of a simple slew rate limiter, which limits the slew rate of only negative going transients to −S. This consists of a subtracter (66), a MAX circuit 68, an adder 70, and a one-sample-delay latch 72. If the positive input to the subtractor is lower than the output by more than S, then the new output equals the previous output minus S.
The two transient conditioners can advantageously be set to different slew rates. Different positive and negative slew rate limits can also be advantageously selected, although such a selection is not shown in FIG. 2. The threshold or thresholds can also advantageously be independently selected.
Referring to
Referring to
Although the present invention has been described in conjunction with the embodiments disclosed herein, it should be understood that the foregoing description is intended to illustrate and not limit the scope of the invention as defined by the claims.
Patent | Priority | Assignee | Title |
7495640, | Mar 12 2001 | INTERDIGITAL CE PATENT HOLDINGS | Reducing sparkle artifacts with post gamma correction slew rate limiting |
7535450, | Feb 19 2002 | INTERDIGITAL CE PATENT HOLDINGS | Method and apparatus for sparkle reduction using a split lowpass filter arrangement |
Patent | Priority | Assignee | Title |
5170152, | Dec 14 1990 | Hewlett-Packard Company | Luminance balanced encoder |
5526060, | Sep 06 1994 | Fairchild Semiconductor | Luma/chroma decoder with demodulated control signal |
5786866, | Oct 15 1996 | Fairchild Semiconductor Corporation | Video color subcarrier signal generator |
6344857, | Apr 02 1998 | HITACHI CONSUMER ELECTRONICS CO , LTD | Gamma correction circuit |
6359663, | Apr 17 1998 | ESTERLINE BELGIUM BVBA | Conversion of a video signal for driving a liquid crystal display |
20020126079, | |||
20020126080, | |||
20020126134, | |||
20030156091, | |||
EP457497, | |||
JP8088770, |
Executed on | Assignor | Assignee | Conveyance | Frame | Reel | Doc |
Feb 19 2002 | Thomson Licensing S.A. | (assignment on the face of the patent) | / | |||
Apr 05 2002 | WILLIS, DONALD HENRY | THOMSON LICENSING S A | ASSIGNMENT OF ASSIGNORS INTEREST SEE DOCUMENT FOR DETAILS | 012998 | /0696 | |
Jul 26 2005 | THOMSON LICENSING S A | Thomson Licensing | CHANGE OF NAME SEE DOCUMENT FOR DETAILS | 051317 | /0841 | |
Jul 30 2018 | Thomson Licensing | INTERDIGITAL CE PATENT HOLDINGS | ASSIGNMENT OF ASSIGNORS INTEREST SEE DOCUMENT FOR DETAILS | 051340 | /0289 |
Date | Maintenance Fee Events |
Apr 09 2009 | M1551: Payment of Maintenance Fee, 4th Year, Large Entity. |
Mar 01 2013 | M1552: Payment of Maintenance Fee, 8th Year, Large Entity. |
Apr 13 2017 | M1553: Payment of Maintenance Fee, 12th Year, Large Entity. |
Date | Maintenance Schedule |
Nov 01 2008 | 4 years fee payment window open |
May 01 2009 | 6 months grace period start (w surcharge) |
Nov 01 2009 | patent expiry (for year 4) |
Nov 01 2011 | 2 years to revive unintentionally abandoned end. (for year 4) |
Nov 01 2012 | 8 years fee payment window open |
May 01 2013 | 6 months grace period start (w surcharge) |
Nov 01 2013 | patent expiry (for year 8) |
Nov 01 2015 | 2 years to revive unintentionally abandoned end. (for year 8) |
Nov 01 2016 | 12 years fee payment window open |
May 01 2017 | 6 months grace period start (w surcharge) |
Nov 01 2017 | patent expiry (for year 12) |
Nov 01 2019 | 2 years to revive unintentionally abandoned end. (for year 12) |